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The truncated multidimensional moment problem: canonical solutions
Classical Analysis and ODEs · Submitted 28 Jun 2024
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is constructed a 1-1 correspondence between canonical solutions and flat extensions of the given moments (both sets may be empty).
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The abstract, sentence by sentence
For the truncated multidimensional moment problem we introduce a notion of a canonical solution. Namely, canonical solutions are those solutions which are generated by commuting self-adjoint extensions inside the associated Hilbert space. It is constructed a 1-1 correspondence between canonical solutions and flat extensions of the given moments (both sets may be empty). In the case of the two-dimensional moment problem (with triangular truncations) a search for canonical solutions leads to an algebraic system of equations. A notion of the index $i_s$ of nonself-adjointness for a set of prescribed moments is introduced. The case $i_s=0$ corresponds to flatness. In the case $i_s=1$ we get explicit necessary and sufficient conditions for the existence of canonical solutions. These conditions are valid for arbitrary sizes of truncations. In the case $i_s=2$ we get either explicit conditions for the existence of canonical solutions or a single quadratic equation with several unknowns. Numerical examples are provided.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | For the truncated multidimensional moment problem we introduce a notion of a canonical solution. | contribution 1.00 | 0.93 | 0.14 | asserted 1.00 |
| s1 | Namely, canonical solutions are those solutions which are generated by commuting self-adjoint extensions inside the associated Hilbert space. | contribution 0.94 | 0.65 | 0.12 | asserted 1.00 |
| s2 | It is constructed a 1-1 correspondence between canonical solutions and flat extensions of the given moments (both sets may be empty). | result 0.84 | 0.90 | 0.32 | asserted 0.99 |
| s3 | In the case of the two-dimensional moment problem (with triangular truncations) a search for canonical solutions leads to an algebraic system of equations. | method 0.51 | 0.78 | 0.06 | asserted 0.98 |
| s4 | A notion of the index $i_s$ of nonself-adjointness for a set of prescribed moments is introduced. | contribution 0.99 | 0.90 | 0.06 | asserted 1.00 |
| s5 | The case $i_s=0$ corresponds to flatness. | interpretation 0.47 | 0.67 | 0.05 | asserted 1.00 |
| s6 | In the case $i_s=1$ we get explicit necessary and sufficient conditions for the existence of canonical solutions. | result 0.93 | 0.91 | 0.18 | asserted 1.00 |
| s7 | These conditions are valid for arbitrary sizes of truncations. | result 0.84 | 0.83 | 0.09 | asserted 1.00 |
| s8 | In the case $i_s=2$ we get either explicit conditions for the existence of canonical solutions or a single quadratic equation with several unknowns. | result 0.94 | 0.93 | 0.11 | asserted 0.79 |
| s9 | Numerical examples are provided. | contribution 0.45 | 0.92 | 0.03 | asserted 1.00 |
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Original abstract
For the truncated multidimensional moment problem we introduce a notion of a canonical solution. Namely, canonical solutions are those solutions which are generated by commuting self-adjoint extensions inside the associated Hilbert space. It is constructed a 1-1 correspondence between canonical solutions and flat extensions of the given moments (both sets may be empty). In the case of the two-dimensional moment problem (with triangular truncations) a search for canonical solutions leads to an algebraic system of equations. A notion of the index $i_s$ of nonself-adjointness for a set of prescribed moments is introduced. The case $i_s=0$ corresponds to flatness. In the case $i_s=1$ we get explicit necessary and sufficient conditions for the existence of canonical solutions. These conditions are valid for arbitrary sizes of truncations. In the case $i_s=2$ we get either explicit conditions for the existence of canonical solutions or a single quadratic equation with several unknowns. Numerical examples are provided.
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